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Magnetic Properties and Electronic Configurations of Mn Ions in the Diluted Magnetic Semiconductor Ba1−xKx(Zn1−yMny)2As2 Studied by X-ray Magnetic Circular Dichroism and Resonant Inelastic X-ray Scattering

Authors :
Suzuki, Hakuto
Zhao, Guoqiang
Okamoto, Jun
Sakamoto, Shoya
Chen, Zhi-Yin
Nonaka, Yosuke
Shibata, Goro
Zhao, Kan
Chen, Bijuan
Wu, Wen-Bin
Chang, Fan-Hsiu
Lin, Hong-Ji
Chen, Chien-Te
Tanaka, Arata
Kobayashi, Masaki
Gu, Bo
Maekawa, Sadamichi
Uemura, Yasutomo J.
Jin, Changqing
Huang, Di-Jing
Source :
Journal of the Physical Society of Japan; 6/15/2022, Vol. 91 Issue 6, p1-5, 5p
Publication Year :
2022

Abstract

The magnetic properties and the electronic excitations of the new diluted magnetic semiconductor Ba<subscript>1−</subscript><subscript>x</subscript>K<subscript>x</subscript>(Zn<subscript>1−</subscript><subscript>y</subscript>Mn<subscript>y</subscript>)<subscript>2</subscript>As<subscript>2</subscript> have been studied by x-ray magnetic circular dichroism (XMCD) and resonant inelastic x-ray scattering (RIXS) at the Mn L<subscript>2,3</subscript> edge. The sum rule analysis of the XMCD spectra yields the net spin moment of 0.45 μ<subscript>B</subscript>/Mn and the small orbital moment of 0.05 μ<subscript>B</subscript>/Mn. This indicates that the Mn atoms are in the high-spin configurations of d<superscript>5</superscript>, whereas the presence of competing ferromagnetic and antiferromagnetic interactions between the Mn ions reduces the net spin moment. RIXS spectra show broad peaks from 1 to 6 eV energy loss, which originate from the d–d crystal field excitations of the Mn ions. Based on a comparison of the RIXS line shapes with those of Ga<subscript>1−</subscript><subscript>x</subscript>Mn<subscript>x</subscript>As, we conclude that the ground state of Mn in Ba<subscript>1−</subscript><subscript>x</subscript>K<subscript>x</subscript>(Zn<subscript>1−</subscript><subscript>y</subscript>Mn<subscript>y</subscript>)<subscript>2</subscript>As<subscript>2</subscript> consists not only of the charge-transferred 3d<superscript>5</superscript>L electron configuration (L: ligand hole) with weakly bound holes as in Ga<subscript>1−</subscript><subscript>x</subscript>Mn<subscript>x</subscript>As, but also of the pure 3d<superscript>5</superscript> configuration with free holes. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00319015
Volume :
91
Issue :
6
Database :
Complementary Index
Journal :
Journal of the Physical Society of Japan
Publication Type :
Academic Journal
Accession number :
157177575
Full Text :
https://doi.org/10.7566/JPSJ.91.064710